Optical Design of a Particulate measurement system

ABSTRACT

The optical design of a measurement system is disclosed. The measurement system comprising a light source configured to provide light along a first axis. The measurement system has a reflecting lens aligned along a second axis where the reflecting lens has a first focus on the second axis and a second focus on the second axis where the second focus is between the first focus and the reflecting lens and where the second focus is positioned near the first axis. The measurement system has a field lens located on the second axis and positioned such that the second focus of the reflecting lens occurs inside the field lens. The measurement system has a relay lens system aligned to the second axis where the relay lens system forms a first focus at the second focus of the reflecting lens. The measurement system has a sensor located on the second axis at a second focus of the relay lens system and is configured to detect scattered light near the second focus of the reflecting lens.

RELATED APPLICATIONS

This application claims the benefit of U.S. provisional application No.60/785,074 filed on Mar. 23, 2006 entitled “Measurement of particulatematter in a media” which is hereby incorporated by reference into thisapplication. This application is related to application “Measurement oflight from a predefined scatter angle from particulate matter in amedia”, “Dual function measurement system”, “Optical design of ameasurement system having multiple sensor or multiple light sourcepaths” and “Self calibrating measurement system” all filed on the sameday as this application and are hereby incorporated by reference.

BACKGROUND OF THE INVENTION

Of interest to the process specialist, engineer, scientist, and others,is the quality or purity of product (media capable of particlesuspension) being manufactured whether it liquid, gas, pharmaceutical,or the like. One measure of product quality is an assay of particulatematter or concentration of particulate matter within the end product orproduct during various stages of production so as to assure thatparticulate matter as a constituent of, or by product of the process,exists at a prescribed amount or within a suitable tolerance. When theparticles in suspension are unknown, the particles may differ incomposition, size, and shape. It is well known that matter interactswith light in a variety of ways, as example by means of absorption,reflection or scatter, and fluorescence to name a few. Various opticalmeans have been devised to measure particulate matter within asuspension such as turbidimeter or nephelometer, particle counter, anddensitometer but all use fundamentally different optical configurationseach designed to measure a specific attribute or concentration range ofthe suspended particles by means of transmittance, reflection, orremittance of light.

Another constraint on the optical measurement configuration is imposedby regulatory agencies or by standardized methods by example the U.S.EPA Method 180.1, ASTM Standard Test Method for Turbidity of Water D1889-00, and by International Standard ISO 7027 for the determination ofturbidity for the assay of water quality. These methods and standardsdictate the geometrical relationship of emitter to detector and thesolid angle of collection optics so as to assure that instrument ofsimilar task perform within designated parameters for reportingpurposes.

Other limitations on devices for nephelometric measurement designed todetermine the presence of particles in a suspension is the ability ofthe device to operate over a wide range of particle sizes andconcentrations without impediment. Particle counters perform well at lowconcentration of particles but are prone to obstruction when theconcentration or particle size becomes greater than the ability of theflow steam to pass through the narrow restriction, orifice, or capillaryof the measurement interrupter. Devices, such as a turbidimeter, withunrestricted flow paths are insensitive to small concentrations ofparticles because the primary measurement technique relies on scatteredlight energy impinging on the detector means is greater than that of theself-generated noise of the detector.

Still another deficiency of devices used in the measure of particles insuspension is a lack of means to evaluate the operational readiness ofthe instrument without disruption of particle flow by the introductionof a calibration standard or calibration device, requiring interactionbetween a skilled operator or technician and the nephelometric device.

The disclosed invention eliminates the need for multiple nephelometricmeasuring devices and also system verification devices in order toperform assay of the presents or absence or number of suspendedparticles in a media as well as verification of the systems ability tomeasure in compliance to required performance attributes.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1—is a sectional view of the optical layout of a particulatemeasurement system in an example embodiment of the invention.

FIG. 2—is a first side view of particulate measurement system in anexample embodiment of the invention.

FIG. 3—is a second side view, with the meniscus lens removed, of aparticulate measurement system in an example embodiment of theinvention.

FIG. 4—is a sectional view of the flow path of a particulate measurementsystem in an example embodiment of the invention.

FIG. 5—is a block diagram of the optical layout of the detection path inan example embodiment of the invention.

FIG. 6—is a block diagram of the optical layout when utilizing more thanone detection path in an example embodiment of the invention.

FIG. 7—is a block diagram of the optical layout of the light source pathin an example embodiment of the invention.

FIG. 7 a to 7 g—are block diagrams of various arrangements andconstructions of an aperture masks used to discriminate angle of scatterfrom particles in suspension in an example embodiment of the invention.

FIG. 8—is a block diagram of the optical layout of the view area of thesuspension media in an example embodiment of the invention.

FIG. 9—is a block diagram of a particulate measurement system utilizinga plurality of light source paths in an example embodiment of theinvention.

FIG. 10—is a block diagram of the optical layout of a particulatemeasurement system with an annulus virtual source and second lightsource in an example embodiment of the invention.

FIG. 11—is a block diagram of the optical layout of a particulatemeasurement system with an uncoated area of the convex lens surface anda second light source in an example embodiment of the invention.

FIG. 12—is a block diagram of the optical detail of an insitucalibration and verification means utilizing light from the primarylight source and optical switching means to divert a portion of theprimary source to the calibration and verification means in an exampleembodiment of the invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENT

FIGS. 1-12 and the following description and exhibit depict specificexamples to teach those skilled in the art how to make and use the bestmode of the invention. For the purpose of teaching inventive principles,some conventional aspects have been simplified or omitted. Those skilledin the art will appreciate variations from these examples that fallwithin the scope of the invention. Those skilled in the art willappreciate that the features described below can be combined in variousways to form multiple variations of the invention. As a result, theinvention is not limited to the specific examples described below, butonly by the claims and their equivalents.

FIG. 1 is a sectional view of the optical layout of a particulatemeasurement system in an example embodiment of the invention.Particulate measurement system comprises: light source 10, flexure mount27, meniscus lens 1, input lens 6, output lens 7, field lens 2, devicebody 19, integrating sphere 11, transmit detector 17, lens 3, aperturemask 9, lens 4; and particle detector 5. Light source 10 is mounted inflexure mount 27 and projects a light along a first optical axis AA.Flexure mount 27 is used to adjust or align the angular relationshipbetween light source 10 and device body 19. A cavity 8 is formed bymeniscus lens 1, input lens 6, output lens 7, field lens 2, and devicebody 19. The media to be tested flows through cavity 8 along an axisperpendicular to the plane of the paper. Gaskets or sealing devices, forexample O-rings, may be used between the lens and the device body tohelp form a fluid tight seal around cavity 8. Output lens 7 is mountedin device body 19 and aligned with first optical axis AA. Integrationsphere 11 is mounted onto device body 19 near output lens 7. Integrationsphere 11 has an entrance port 15 aligned with the first optical axis A.Transmit detector 17 is mounted substantially 90 degrees to entranceport 15 at an exit port 16 of integrating sphere 11. Meniscus lens 1,field lens 2, lens 3, aperture mask 9, and lens 4 are aligned along asecond optical axis BB. Particle detector 5 is mounted to device bodyand aligned with the second optical axis BB. The inside surface 12 ofintegrating sphere 11 may be preferentially coated to alter thereflectivity or enhance stability, durability, or maintainability of thereflective surface.

FIG. 2 is a first side view of particulate measurement system in anexample embodiment of the invention. Light source 10 may be that of alaser, LED, (Light Emitting Diode), incandescent lamp, or dischargelamp, or any other source of coherent or non-coherent radiation capableof stimulating the detector to produce useful information. The ingress41 and egress 44 of a flow through the nephelometric device is carriedby inlet tube 40 and outlet tube 43 facilitated by connection 39 and 42attached to device body 19. A section view of clamp 33 in FIG. 2 showsthe means by which screw 36 applies force to clamp 33 to squeezedetector sleeve 32 to secure detector holder 34 to a fixed position.

FIG. 3 is a second side view, with the meniscus lens removed, of aparticulate measurement system in an example embodiment of theinvention.

FIG. 4 is a sectional view of the flow path of a particulate measurementsystem in an example embodiment of the invention. Particulatemeasurement system comprises: meniscus lens 1, output lens 7, field lens2, device body 19, lens 3, aperture mask 9, lens 4, particle detector 5,inlet tube 40 and outlet tube 43. The ingress 41 and egress 44 of a flowthrough the nephelometric device is carried by inlet tube 40 and outlettube 43 facilitated by connection 39 and 42 attached to device body 19.O-ring seals 45 and 46 seal tubing 43 and 40 to device body 19. Thefirst optical axis AA forms a line perpendicular to the paper and iscentered in output lens 7.

FIG. 5 is a block diagram of the optical layout of the detection path inan example embodiment of the invention. FIG. 5 shows light scattered inthe direction of meniscus lens 1 by particles in suspension media 47 atobject plane 49. Meniscus lens 1, field lens 2, and lenses 3 and 4 alongoptical axis BB form an erect image at image plane 49″ of the particlelocated at object plane 49. An intermediate image of the particles isformed by meniscus lens 1 along optical axis BB at image plane 49′,within field lens 2. By forming the intermediate image within field lens2 only that light which is reflected, scattered or emitted fromparticles toward meniscus lens 1 are brought to focus at image plane49″. As result, no image of particles in suspension is formed as directresult of lenses 3 and 4, but only as result of light impinging uponmeniscus lens 1.

In one example embodiment of the invention, meniscus lens 1 is anemersion lens of refracting material greater than the refractive indexof the suspension media. Meniscus lens 1 has a concave refracting firstsurface in contact with the suspension media, and a convex reflectingsecond surface. The first and second surfaces need not be concentric andneither surface needs be concentric with object plane 49. In one exampleembodiment of the invention the first refracting surface of meniscuslens 1 may be inert to the suspension media. Because the secondreflecting surface of meniscus lens 1 is protected by the firstrefracting surface, meniscus lens 1 may be cleaned without danger ofdamaging the more delicate reflecting surface. The first refractingsurface allows for an additional degree of freedom in the correction ofoptical aberrations that may otherwise degrade the image quality atimage planes 49′ and 49″ without need of aspheric surfaces to theadvantage of lower production cost. Because the main optical power ofthe meniscus lens is provided by the reflecting surface, problems withdispersion over a wide range of test wavelengths may be minimized.Marginal ray 50 from object plane 49 is refracted by the concave surfaceof meniscus lens 1, and propagates as ray 50 a to reflective convexsurface of meniscus lens 1. Upon reflection on the coated convex surfaceof the lens the reflected ray 50 b is again refracted by the concavesurface of the meniscus lens 1 and exits the lens as refracted ray 50 c.Because object plane 49 and intermediate image plane 49′, within fieldlens 2, are displaced along optical axis BB little refraction takesplace on either side of field lens 2 as the index of refraction betweensuspension media 47 and index of refraction of field lens 2 are similarand the intermediate image 49′ is concentric, or nearly so, to theconvex surface of field lens 2. Meniscus lens 1 provides a largenumerical aperture that captures a large portion of the light scatteredfrom a particle in suspension media 47. In one example embodiment of theinvention, in excess of 1/7 of the total scattered light may be utilizedto impinge upon particle detector 5 at image plane 49″. Marginal ray 50c is refracted by lens 3, as marginal ray 50 d, and emerges from lens 3as marginal ray 50 e. Field stop 9 defines the extent to which marginalrays scattered from particle in suspension media 47 will propagatethrough the optical system. An image of field stop 9 is formed at ornear the surface of meniscus lens 1 as field stop image 9′. Marginal ray50 e propagates to lens 4 and is refracted as marginal ray 50 f,emerging from lens 4 as marginal ray 50 g where an erect image of theparticle is formed from the scatted light from object plane 49 at imageplane 49″. Principle ray 51 follows a similar path through the opticalsystem passing through the center of field stop 9 and also through thecenter of the image 9′ of the field stop formed at the surface ofmeniscus lens 1. Field stop 9 is positioned from lens 4 such thatparticle detector 5 is at the infinite conjugate of field stop 9. Thus,any portion of the image formed at field stop 9 impinges equally at thesurface of particle detector 5.

Detector 5 may be that of a photodiode, Photo-Multiplier Tube (PMT),Charged Coupled Device (CCD) or Complementary Metal Oxide Semiconductor(CMOS) image sensor, or any other means to convert light or radiationinto quantifiable values of electrical potential or current. In oneexample embodiment of the invention, area array detectors such as CCD orCMOS image sensors may be used to measure by spatial position andincremental area the intensity of the image formed on the image sensor.Using this information, the device may measure size, shape,distribution, occurrence, and velocity of the particles in suspension atobject plane 49. The magnification of object to image along optical axisBB is selected to provide adequate resolution for the measurements ofinterest and defines the maximum area that can be measured in thesuspension. If the size of the image sensor is 6.4×4.8 mm and themagnification of the optical system is 2×, then the maximum area thatcan be measured in the suspension is 3.2×2.4 mm. For a given imagesensor a fixed number of photosensitive sites are present as example640×480 pixels, therefore each pixel is 10 um and represents aresolution of 5 um object per pixel in suspension. If the particles tobe measured are at least 2 to 3 times larger than the resolution of thesystem, then a reasonable measure of the size and shape of the objectcan be determined. The depth of the image along optical axis BB is aresult of the diameter or width of the illuminating beam along opticalaxis BB and, or the depth of field of the imaging optical system. Adefined measurement volume may be determined using the width of theillumination along optical axis BB, the depth of field of the imagingoptical system, the magnification of the optical system, and the size ofthe particle detector. A count of the illuminated particles orfluorescent particles within the defined measurement volume may bereported as a count per cubic millimeter. If the image sensor is of anintegrating type, as the case for CCD and CMOS image sensors, theintegration time—the time allotted for charge to accumulate on thephotosensitive area of the device, may be used to determine the flowrate of the particles in suspension by measure of the number of pixelstransgressed during the integration period. The resulting image issometimes referred to as a “streak”, the length of which and the knownintegration time can be used to calculate the velocity of the particle,hence the flow rate of the suspension media. When the concentration ofparticles in suspension is sufficiently high, individual particlesbecome indistinguishable at the image sensor but may be measured as aconcentration of particles by means of the total charge accumulatedduring the known integration period on the image sensor, or amperecurrent product of particle detector 5 as that of a photodiode, that iscorrelated to Nephelometric Turbidity Units (NTU), FormazinNephelometric Unit (FNU), McFarlane Units, or other standardnephelometric unit of measure of the cloudiness or haze of thesuspension calibrated to a known concentration of nephelometricstandard.

The disclosed invention is not limited to a single detection path. FIG.6 is a block diagram of an optical layout when utilizing more than onedetection path in an example embodiment of the invention. A secondoptical axis CC is introduced at substantially 90 degrees to opticalaxis BB, both at substantially 90 to the optical axis of the lightsource. Light scatter from particle at object plane 49 is collected andtransmitted along optical axis CC in the same manor as described forthat of FIG. 5 utilizing instead meniscus lens 1A, field lens 2A, lenses3A and 4A, to form an erect image of the particle at particle detector5A. The two images are related, as the image formed at particle detector5A is the image profile of the image formed at particle detector 5. Inaddition the two detectors, 5 and 5A need not have the same spectralresponse nor is there a need for meniscus lens 1 and 1A to have the samespectral reflectivity. Indeed each optical path may be altered by theaddition of optical filters or by means of coating reflectivity or bydetector response such that each optical path is sensitive to differentportion of the spectra so as to detect absorption or emission fromparticles in suspension media 47 at object plane 49 at uniquewavelength(s).

FIG. 7 is a block diagram of the optical layout of the light source pathin an example embodiment of the invention. It is desired to keep strayradiant energy from propagating along optical axis BB to particledetector 5. It is therefore best practice not to illuminate more of thesample volume than that which can be imaged on to particle detector 5.Input lens 6 focuses light 53 as 53 a from light source 10 to illuminatethat sample volume to which will contribute an image of the samplevolume at particle detector 5. After light has propagated through thesample volume, output lens 7 directs the transmitted light, not absorbedor scattered by the particles in suspension as light 53 b, into theentrance port 15 of integrating sphere 11. Coatings or finish on theinside surface 12 of the integrating sphere 11 are optimized to bediffusely reflective so as to uniformly illuminate the inside surfacesof the integrating sphere with the transmitted light. In so doingtransmit detector 17 will measure the same intensity of light regardlessof the exact angle or distribution of light within the transmit beam oflight source 10 along optical axis of illumination AA. Exit port 16 inthe integrating sphere 11 is positioned at substantially 90 degrees tothe entrance port of integrating sphere 11. So as to prevent directillumination of transmit detector 17 and thus reduce the sensitivitiesto beam incidence and position, the lines of sight of the detector 54and 54 a of the transmit detector 17 does not include entrance port 15or the incident transmit energy on the inside surface 12 of integratingsphere 11. Signals generated from transmit detector 17 and particledetector 5 can be utilized to determine the ratio of transmitted lightto scatted light or to measure the absorption or fluorescence ofparticles. Another advantage of the novel use of an integrating spherefor the measure of transmitted light in a nephelometer is due to theredistribution of light across the inner surface 12 of integratingsphere 11, resulting in a decrease in surface intensity at the transmitdetector 17, thereby eliminating the need for light traps or neutraldensity filters to reduce the maximum value for incident light impingingon the transmit detector 17.

A unique quality of the disclosed invention is the ability to image anobject or mask, positioned along optical axis BB at field stop 9, ontoor near the surface of meniscus lens 1. As shown in FIG. 7 a, an annularmask 9 a place at the location of field stop 9, is utilized todiscriminate by permissible propagation only those rays which arereflected or scattered from object plane 49 at a high angle relative tooptical axis BB. Annular masks 9 b and 9 c used in lieu of stop 9 areutilized to change the permissible propagation angle of scatter whilemaintaining a constant optical system etendue. Etendue is used tospecify the geometric capability of an optical system to transmitradiation, its throughput. The numeric value of the etendue is typicallya constant of the system and gets calculated as the product of theopening size and the solid angle that the system accepts light from.Etendue may also be known as tie collecting or light gatheringcapability of an optical system. An iris diaphragm, as shown in FIG. 7b, substituted for fixed field stop 9 of FIG. 7 can be adjusted to alterthe amount of light impinging on particle detector 5 and also the totalincluded angle of scatter from object plane 49. Light scattered from aparticle(s) towards the incident beam of illumination is referred to as“back scatter” in nephelometric terms. Conversely, light scattered awayfrom the source of illumination is referred to as “forward scatter”.Light scattered from a particle neither toward or away from the incidentlight source is referred to as “side scatter” in nephelometric terms.Apertures or masks in the forms as shown in FIG. 7 c through FIG. 7 gpermit measurement of the amount, by scatter type, of light scatted froma particle(s). This is useful so as to be able to measure differentconcentrations of particles, as different types of scatter are moreuseful as to linearity or sensitivity depending on the concentration ofparticle(s) in the suspension media. A circular mask offset from opticalaxis BB placed at the position of field stop 9 of FIG. 7, as in FIG. 7c, is rotated eccentric to optical axis BB as 9 a, 9 b, and 9 c, to keepconstant the etendue of the optical system with preferential selectionof the scatter angle about optical axis BB as a conic section. Twosemi-circular masks rotated independently about optical axis BBlaminated in close proximity to one another at the position of fieldstop 9 of FIG. 7 is shown as 9 a, 9 b, 9 c, and 9 d in FIG. 7 d.Rotation of the masks independently creates a sector aperture throughwhich a portion of scattered light about optical axis BB is permitted topass through the optical system to particle detector 5 at the selecteddirection of scatter. A mask in the form of a shutter(s) is utilized toselect an angular portion of the scatted or emitted light from objectplane 49 as shown in FIG. 7 e. A shutter is slide across the face ofaperture 9 of FIG. 7 to preferentially transmit or block the propagationof rays to particle detector 5 dependent on the angle of scatter ofemission from object plane 49. The shutter in position 9 a of FIG. 7 etransmits light that is forward scattered from object plane 49. Twoshutters independently adjustable orthogonal to each other laminated inclose proximity at the position of field stop 9 of FIG. 7 is shown inFIG. 7 f. The aperture, a sector, formed by the two shutters can betranslated off optical axis BB unlike that of the sector formed by thesemi-circular masks of FIG. 7 d. A pixilated mask at position of fieldstop 9 controlled by means of selective polarization of the scatteredlight passing through a polarizing film and electrically polarizedliquid crystals as in a transmission LCD, (Liquid Crystal Display), isutilized to block, by means of cross polarization, light frompropagating through said LCD along optical axis BB. A pixilated mask canbe substituted for any or all of the described forms of aperturespreviously described without preference. The choice of the maskeffectively selects the angles of reflection that detector 5 willeventually process. Alternately, when only the angle and or intensity ofscattered or emitted light is to measured from object plane 49 and noimage need be formed of the scattering particle(s), as in the case ofpresence of particles or fluorescence, then a image array such as a CCDor CMOS image plane sensor is placed in substitution to field stop 9 asshown in FIG. 7 g. Light impinging on pixels of the image plane sensoris thus discriminated by angle of scatter or emission since an image ofthe pixel is formed at the surface of meniscus lens 1 as field stopimage 9′. Using the optical layout having multiple detection paths asshown in FIG. 6, multiple masks may be used having different maskingareas, such that different measurements of the angle of scatter forparticles may be made simultaneously.

FIG. 8 is a block diagram of the optical layout of the view area of thesuspension media in an example embodiment of the invention. Light fromlight source 10 propagates as marginal ray 53 to input lens 6 to form acaustic of illumination or focused image of the source at the objectplane 49. Light not scattered or absorbed continues along optical pathAA to exit lens 7 where upon the unabsorbed or light not scattered byparticulate matter is relayed to inside surface 12 of integrating sphere11 through input port 15. Alternately lenses 6 and 7 need not haveoptical power in the case where the light being emitted into thesuspension media is collimated or focused and the subtended angle intointegrating sphere is small. Lenses 6 aid 7 may be completely removed inthe case where the suspension media need not be isolated from theexternal elements of the device, for example when the particles aresuspended in air or some other gas or vapor.

In one example embodiment of the invention, a plurality of illuminationpaths may be used. FIG. 9 is a block diagram of a particulatemeasurement system utilizing a plurality of light source paths in anexample embodiment of the invention. FIG. 9 has light sources 10, 10 aand 10B projecting illumination along optical axis 52, 52A, and 52B. Inone example embodiment of the invention light source 10, 10A and 10Bneed not have the same spectral emission or may have selectedwavelength(s) of emission of by the introduction of optical filtermaterial along optical axis 52, 52A, or 52B, or by judicial selection ofoptical materials or coatings used for lenses 6, 6A, 613 and, or lenses7, 7A, and 7B.

Another aspect of the present invention is the ability to introducelight into the detection path(s) of a known amount or percentage so asto facilitate the calibration or verification the operational readinessof the device without disruption to the flow or particle stream. Anon-disruptive calibration or verification is accomplished by theintroduction of light within the field of view of the detection opticsalong optical axis BB at the image plane of the field stop 9′,synonymous to the surface of meniscus lens 1, as shown in FIG. 10.Annular waveguide 60, of transparent plastic, glass, or other suitablematerials, transports light from second light source 56 along opticalaxis 59 between the two face surfaces by means of Total InternalReflection, (TIR), from outer edge of annular waveguide 60 to inner edgeof annular waveguide 60. The inner edge of annular waveguide 60 may bepreferentially ground, etched, or coated so as to scatter light alongoptical axis BB as an annulus of marginal rays to form an image ofannular waveguide 60 at field stop 9 and subsequently impinges equallyonto particle detector 5 since particle detector is at the infiniteconjugate of lens 4. By selectively permitting second light source 56 toemit light at a known intensity, by provision of electrical ormechanical means, light is introduced along optical axis BB in additionto light scattered or emitted from particles stimulated by light source10. Since light introduced by light source 10 must travel through thesuspension media the light is affected by the concentration of particlesin the suspension media by means of absorption, scatter, and emission oflight in the same manor as the transmitted light from light source 10 totransmit detector 17. The ratio of the amount of transmitted light todetector 17 from light source 10 to the amount of light transmitted fromsecond light source 56 to particle detector 5 is constant provided lightsource 10 and second light source 56 emit at a constant intensity andthat all optical surfaces degrade in like manor. An abnormal conditionexists as result of the ratio from the established value is in deviationby more than a prescribed amount as to warrant action for eithercorrection of the abnormal condition or to compensate of the ratio so asto restore the ratio to the established value.

Since lenses 3 and 4 relay an image from within field lens 2 it is alsopossible to utilize this arrangement to opt for a material orconstruction for field lens 2 that will partially scatter by appliedelectrical field or other stimulation cause field lens 2 to changeoptical characteristics to the objective as to redirect light emittedinto the edge of field lens 2 by means of scatter or to emit lightwithin field lens 2 along optical axis BB and thus impinge upon particledetector 5. This arrangement has the advantage of the light scattered oremitted is unimpeded and not transmitted through the suspension mediaand is unaffected by biological films or depositions of materials thatcome in contact with the suspension media, thus a more stable andreproducible calibration or verification source is result.

Alternately light may be introduced along optical axis BB through acentral uncoated portion or aperture 58 in the optical coating of theconvex surface of meniscus lens 1 as shown in FIG. 11. An image ofsecond light source 56 is brought to focus at the concave surface ofmeniscus lens 1 synonymous with image 9′ of field stop 9, by lens 57through the uncoated central aperture 58 in meniscus lens 1. Thealternate scheme for the introduction of light from a second lightsource differs from the previously described method of FIG. 10 since nophysical radiator is present at concave surface of meniscus lens 1 butinstead an image of second light source 56, and that the light comprisedof principle rays and not marginal rays. The light impinging on particledetector 5 is however indistinguishable in result between the method oflight introduction of FIG. 10 and FIG. 11 as both effectively emit lightat image plane 9′ of field stop 9 within the field of view of thedetection optics along optical axis BB.

Another means to introduce light along the optical axis BB for thepurpose of calibration or verification of operational readiness isdisclosed for the present invention without the need for a second lightsource is shown in FIG. 12. Light from light source 10 is emitted alongoptical axis BB through input lens 6 and output lens 7 through inputaperture 15 of integrating hemisphere 13 to impinge on the insidesurface 12 of integrating sphere 11. Light is diffusely reflected bymultiple incidences between inside surface 12 of the integrating sphereto emerge along optical axis 55 at exit aperture 16 of integratingsphere 11. Optical surface 62, by example selectable by rotation aboutaxis of rotation 63 with at least one transmitting surface or aperture64 and at least one reflecting area 62 is positioned beyond the exitaperture 16 of integrating hemisphere 13 to reflect light substantially90 degrees to optical axis 55 along optical axis 68 or transmit lightalong optical axis 55 dependent upon the alignment of aperture 64 orreflecting area 62 to optical axis 55. Positioning of reflecting surface62 along optical axis 55, reflects light emerging from exit aperture 16to impinge upon transmit detector 17 positioned along optical axis 68,thus a measure of the transmitted light from light source 10 isascertained. Positioning aperture 64 along optical axis 55 permits thetransmission of light along optical axis BB through central aperture 58of meniscus lens 1 by relay of emitted light from exit aperture 16through aperture stop 65, lens 66, optical fiber 67, and lens 57. Animage of the end of optical fiber 67 is formed at the concave surface ofmeniscus lens 1 through central aperture 58 synonymous to the image 9′of field stop 9, to impinge upon particle detector 5 in proportion tothe light detected by transmit detector 17 by means of field lens 2, andlens 3, field stop 9, and lens 4.

1. A measurement system comprising: a light source configured to providelight along a first axis; a reflecting lens aligned along a second axiswhere the reflecting lens has a first focus on the second axis and asecond focus on the second axis where the second focus is between thefirst focus and the reflecting lens and where the second focus ispositioned near the first axis; a field lens located on the second axisand positioned such that the second focus of the reflecting lens occursinside the field lens; a relay lens system aligned to the second axiswhere the relay lens system forms a first focus at the second focus ofthe reflecting lens; a sensor located on the second axis at a secondfocus of the relay lens system and configured to detect scattered lightnear the second focus of the reflecting lens.
 2. The measurement systemof claim 1 where the first axis is perpendicular to the second axis. 3.The measurement system of claim 1 where the field lens is made from amaterial having a index of refraction similar to that of a suspensionmedia flowing through the measurement system.
 4. The measurement systemof claim 1 where the reflecting lens is a meniscus lens having a firstrefracting surface and a second reflecting surface.
 5. The measurementsystem of claim 4 where the first refracting surface and the secondreflecting surface of the meniscus lens are spherical.
 6. Themeasurement system of claim 4 where the first refracting surface and thesecond reflecting surface of the meniscus lens are not concentric. 7.The measurement system of claim 4 where the meniscus lens is made from amaterial having a index of refraction greater than that of a suspensionmedia flowing through the measurement system.
 8. The measurement systemof claim 1 further comprising: an aperture stop located in the relaylens system where the field lens is configured to focus an image of theaperture stop onto the reflecting lens.
 9. The measurement system ofclaim 1 where the sensor has a plurality of active areas where eachactive area converts light into charge.
 10. The measurement system ofclaim 1 further comprising: a processor coupled to the sensor andconfigured to determine at least one of the following: a particle countper unit volume, turbidity, a flow rate of a suspension medium.
 11. Themeasurement system of claim 1 further comprising: an integration spherehaving a entrance port and an exit port where the integration sphere ison the first axis opposite the light source and the entrance port isaligned with the first axis; a detector aligned with the exit port andconfigured to detect the intensity of light in the integration sphere.12. The measurement system of claim 11 where the entrance port ispositioned substantially 90 degrees with respect to the exit port.
 13. Amethod for measuring scattered light, comprising: illuminating a samplevolume along a first axis where the sample volume contains particulatessuspended in a medium; focusing light scattered from the particulatessuspended in the medium along a second axis to an intermediate imageusing a reflecting surface where the intermediate image is locatedinside a field lens; focusing the intermediate image onto a sensor usinga lens system.
 14. The method for measuring scattered light of claim 13further comprising: blocking a portion of the light scattered from theparticulates suspended in the medium where the blocked portion isdependent on the angle of scattered light.
 15. The method for measuringscattered light of claim 13 where the first axis is perpendicular to thesecond axis.
 16. The method for measuring scattered light of claim 13where the reflecting surface is on a meniscus lens having a firstrefracting surface and a second reflecting surface.
 17. A measurementsystem, comprising: a light source directed along a first axis andconfigured to illuminate a sample volume where the sample volumecontains particulates suspended in a medium; an integration spherehaving an entrance port and an exit port where the entrance port islocated on the first axis opposite the light source and the integrationsphere is configured to collect the light from the light source passingthrough the sample volume; a sensor aligned with the exit port andconfigured to detect a light amount collected by the integration sphere.18. The measurement system of claim 17 where the entrance port ispositioned substantially 90 degrees with respect to the exit port. 19.The measurement system of claim 17 where the entrance port is not in afield of view of the sensor.